ATESO LABS // RESEARCH & PEER-REVIEW ARCHIVE
← Back to Publications Index Falsification Ledger
TIER 1 MAPPED · WHITE PAPER 04
SHA-256: 0f5f6572f15d3fd7d610ddd24ab6560af1af77831ed7f60cbd73c8febdb0c7c8

Sub-Cycle Grid Defense: Sub-Cycle Micro-Shedding, Inverter Coordination, and Millisecond Frequency Regulation in High-Density AI Campuses

The grid cannot sustain AI as a shock load. Computing must become the damper.

Author: Brennan DeCrow
Affiliation: ATESO Labs / ManyMoats Research
Parent Research Authority: ATESO & The Magma Runtime: The Thermodynamic Obsolescence of Document-Centric Execution for Continuous Spatial Compute (DeCrow, 2026; USPTO Provisional App #64/159,586, Claims 5, 14, 15, 19) [1]
Status: M-Tier Master White Paper. Gold Master Candidate (post-Stage 5 synthesis, 22 September 2026; supersedes v3.2)
Review lineage: physics seat → spatial seat → systems seat → long-context seat → synthesis seat
Next stage: Seat A & Seat B final stamp

Evidence notation (shared across the White Paper series). F formal result under stated assumptions · R reproduced from an executable artifact, including simulation · U author-reported, raw data not in the package · V independently checked against a grid operator, standards body, vendor or published third-party source · P proposed design or experiment not yet run. Appendix A assigns a mark to every load-bearing number.


┌────────────────────────────────────────────────────────────────────────────────┐
│                              THE EXECUTIVE STRIP                               │
├───────────────────┬────────────────────┬─────────────────────┬─────────────────┤
│ TRIGGER           │ FULL SHED          │ PRODUCT             │ FLOOR           │
│ 59.85 Hz          │ 45 MW in 1 cycle   │ ERCOT FFR           │ 59.30 Hz        │
│ ERCOT FFR setpoint│ 35–52 ms end to end│ ≤ 15 cycles allowed │ first UFLS stage│
│                   │ 5–7× inside ERCOT  │ 15-min compute hold │ (5% of load)    │
└───────────────────┴────────────────────┴─────────────────────┴─────────────────┘

Abstract

AI training campuses swing tens of megawatts in lockstep as thousands of accelerators alternate between compute and communication [15]. The grid has noticed. NERC documented 1,500 MW of data-center load dropping off the Eastern Interconnection in a single event [14]. Texas now requires loads of 75 MW or more to accept disconnection in emergencies [13]. ERCOT is tracking about 410 GW of large loads seeking interconnection, some 87% of them data centers [6].

ATESO turns that liability into a resource. Its Compute-As-Virtual-Inverter (CAVI) sheds deferrable compute within one AC cycle of a trigger: 45 MW at 2.70 MW/ms, inside a 3.0 MW/ms bus cap. It then holds the curtailment for fifteen minutes entirely within the compute fabric. It adds no battery, cycles no cells, and leaves the facility UPS on float.

On a 1 GVA islanded system with H = 3 s, a 100 MW step drives the rate of change of frequency to 1.00 Hz/s. There, a frequency-response model shows the shed lifting the nadir from 59.20 Hz, below ERCOT’s first under-frequency load-shedding stage at 59.30 Hz, to 59.54 Hz. On ERCOT’s bulk system, the same 45 MW offsets 3.3% of the loss of a 1,375 MW unit.

End to end, the response completes in 35–52 ms, 5–7× inside ERCOT’s 15-cycle requirement for Fast Frequency Response.

We also report where the argument stops: - Magnitude sets the nadir more than speed does. Delivering the same 45 MW at fifteen cycles instead of one costs only 28 mHz here. - Equivalent inertia depends on the window over which it is measured. - Sub-synchronous stability requires an impedance scan against the real network.


The Grid Anchor

Electrical & grid metric Conventional AI hyperscale campus ATESO Compute-As-Virtual-Inverter (CAVI) Grid & financial impact
Transient power ramp 50–150 MW in < 100 ms
(di/dt > 1.5 kA/s at 138 kV)
≤ 3.0 MW/ms bus cap
45 MW shed at 2.70 MW/ms
Bounded inductive transient
L·di/dt = 57.1 V at 13.8 kV (0.060% of BIL)
Frequency response latency None
(volatile load)
One-cycle actuation (16.7 ms)
35–52 ms end to end
ERCOT FFR-capable
5–7× inside the 15-cycle requirement; 15-minute hold
Interconnection pressure ERCOT large-load queue ≈ 410 GW
(≈ 87% data centers, Mar 2026)
Designed to support NERC BAL-003-2
and ERCOT FFR; complements Texas SB 6
Strengthens the interconnection case
a controllable load, not a shock load
Equivalent inertia H = 0 s
(no rotating mass)
HE = 4.20 s on 100 MVA
(420 MW·s, first 155.5 ms, 0.5 Hz basis)
≈ a 105 MVA unit at H = 4 s (energy)
≈ a 250 MW unit’s 18% governor headroom (power)
Incremental storage CAPEX ≈ $85M
(dedicated 100 MW / 200 MWh BESS)
$0
(hold is compute-internal)
≈ $85M avoided
Electrochemical wear Cycle-limited
(every event ages cells)
Zero cell cycling
(UPS stays on float)
No new NFPA 855 installation

*ATESO CAVI is designed to support Balancing Authority frequency response under NERC BAL-003-2 [2] and to qualify as an ERCOT Load Resource providing Fast Frequency Response [4, 7]. Its continuous droop tier maps onto ERCOT’s Controllable Load Resource primary frequency response. In PJM it maps onto Regulation and Synchronized Reserve (§4.8). IEEE Std 2800-2022 [8] and IEEE Std 1547-2018 [9] do not govern loads. ATESO adopts their active-power–frequency provisions by analogy, as a voluntary standard of care.


1. The AI Grid Shock: The Physics of di/dt and RoCoF

1.1 Why the grid now treats AI as a shock load

The binding constraint is not energy alone. It is the rate of change of power: the di/dt that a campus imposes on the network.

1.2 The synchronous step load

Collective operations such as AllReduce and tensor-parallel barriers move processors from memory stalls to full-throttle matrix multiplication together.

[Fig. 1 — The high-density AI transient]

   140 MW ──┐                      ▲ collective step: +100 MW in < 50 ms
            │                     ╱
            │                    ╱
    40 MW ──┴───────────────────┘
            0 ms                50 ms               100 ms

1.3 Rate of change of frequency, and the two grids this paper addresses

Frequency obeys the per-unit swing equation [19]:

2Hsysf0dfdt=Pmech−PelecSn[p.u.] \frac{2H_{\text{sys}}}{f_0}\,\frac{df}{dt} \;=\; \frac{P_{\text{mech}} - P_{\text{elec}}}{S_n}\qquad[\text{p.u.}]

Here Hsys is the system inertia constant (s), f0 = 60 Hz and Sn the system base (MVA). The initial rate of change of frequency (RoCoF) for a power imbalance ΔP is therefore:

RoCoF=|dfdt|=f0ΔP2HsysSn \text{RoCoF} \;=\; \left|\frac{df}{dt}\right| \;=\; \frac{f_0\,\Delta P}{2\,H_{\text{sys}}\,S_n}

Case A: the islanded system. An isolated sub-transmission island or industrial microgrid with Sn = 1,000 MVA and Hsys = 3.0 s:

RoCoF=60Hz2×3.0s×1,000MVA×100MW=1.00Hz/s \text{RoCoF} \;=\; \frac{60\ \text{Hz}}{2 \times 3.0\ \text{s} \times 1{,}000\ \text{MVA}} \times 100\ \text{MW} \;=\; 1.00\ \text{Hz/s}

Steps of 150–250 MW on the same island reach 1.5–2.5 Hz/s. The case applies to any system that runs, or can become, electrically separate, such as a transmission pocket after it islands from the interconnection. While a pocket remains synchronously connected, its frequency is the interconnection’s frequency.

Case B: the ERCOT bulk system. ERCOT sets its critical inertia at 100 GW·s; the lowest it recorded through 2017 was 130 GW·s [5]. Stored kinetic energy replaces HsysSn: - A 100 MW step then moves frequency at only 0.023–0.030 Hz/s. - ERCOT’s design contingency, the simultaneous loss of both South Texas Project units (2,750 MW), moves it at 0.64–0.83 Hz/s. - ERCOT requires that frequency not fall from 59.7 Hz to 59.3 Hz in less than 0.416 s after that loss [5].

The floor. If frequency reaches 59.30 Hz, ERCOT’s first under-frequency load-shedding (UFLS) stage sheds 5% of system load [5], as required under NERC PRC-006 [3].

On an island, a single campus can decide whether that floor is reached (§4.4). On the bulk system, a single campus is one contributor to the fleet that defends it (§4.5).


2. Inverter Coordination vs. the Limits of Chemical Buffering

Utilities increasingly ask large loads to firm themselves with dedicated battery energy storage (BESS).

──────────────────────────────────────────────────────────────────────────────────────
BUFFER                        CAPEX (100 MW)     CYCLE WEAR              NEW FIRE-CODE FOOTPRINT
──────────────────────────────────────────────────────────────────────────────────────
Chemical BESS (100 MW/200 MWh) ≈ $85M             Every event ages cells  NFPA 855 installation
ATESO CAVI compute damper      $0 incremental     None (UPS on float)     None
──────────────────────────────────────────────────────────────────────────────────────

2.1 What a dedicated battery costs

2.2 Where batteries still win

Batteries follow bidirectional, energy-neutral signals without touching the host’s workload. They can also inject power. CAVI can only withhold it. This paper does not claim that CAVI replaces storage for every service; it claims CAVI makes storage unnecessary for fast under-frequency response.

2.3 The CAVI advantage

CAVI draws its response from work that can wait. The shed comes from deferring Class B computation, not from a battery. No cells cycle, no capital is added, and the facility UPS remains on float, reserved for utility-outage ride-through.


3. Compute-As-Virtual-Inverter (CAVI) via Granular Micro-Shedding

ATESO treats compute as discrete, resident binary granules governed by a sub-millisecond admission loop (h ≤ 1 ms), not as opaque operating-system tasks. That structure lets the runtime modulate active power the way an inverter would: precisely, quickly and on command.

3.1 Workload partitioning and shedding capacity

3.2 Campus topology

[Fig. 2 — Campus electrical topology and the damping boundary]

  138 kV transmission bus (utility intertie)
         │
         ▼
  2 × 100 MVA, 138 / 13.8 kV substation transformers
  (X_leak = 0.10 pu → L_leak = 0.505 mH referred to 13.8 kV · BIL 95 kV)
         │
         ▼
  800 V DC facility bus · 45 MW shed = 56,250 A
         │
         ├── Accelerator socket 1 ──> 0.5625 A at 800 V (≈ 562 A at the 0.8 V core rail)
         ├── Accelerator socket 2 ──> 0.5625 A at 800 V
         └── … 100,000 sockets ─────> desynchronized ramp: 2.70 MW/ms (cap 3.0 MW/ms)

3.3 Socket-level current

Spread across 100,000 accelerator sockets, a 45 MW shed is 450 W per socket: - On the 800 V bus, that is 0.5625 A per socket. - At the socket’s core rail, near 0.8 V, it is about 562 A. Ramped over one cycle, that is 0.034 A/µs.

The same voltage regulators already follow compute-to-communication transitions every training iteration [15]. A ramp that spreads the change across a full AC cycle adds no new stress to the voltage regulators.

3.4 Transformer inductive transient (IEEE C57.12.00)

Consider the worst case: the entire 45 MW shed passes through one 100 MVA, 13.8 kV transformer with leakage reactance 0.10 p.u.

ΔI=45×106W3×13,800V=1,882.7Adidt=1,882.7A(1/60)s=1,882.7A0.01667s=112,960A/s=113.0kA/s \Delta I = \frac{45 \times 10^6\ \text{W}}{\sqrt{3}\times 13{,}800\ \text{V}} = 1{,}882.7\ \text{A} \qquad \frac{di}{dt} = \frac{1{,}882.7\ \text{A}}{(1/60)\ \text{s}} = \frac{1{,}882.7\ \text{A}}{0.01667\ \text{s}} = 112{,}960\ \text{A/s} = 113.0\ \text{kA/s}

Zbase=(13,800)2100×106=1.9044ΩXleak=0.19044ΩLleak=0.190442π×60=0.505mH Z_{\text{base}} = \frac{(13{,}800)^2}{100\times10^6} = 1.9044\ \Omega \qquad X_{\text{leak}} = 0.19044\ \Omega \qquad L_{\text{leak}} = \frac{0.19044}{2\pi\times 60} = 0.505\ \text{mH}

VL=Lleakdidt=0.50516mH×112,960A/s=57.1V V_L = L_{\text{leak}}\,\frac{di}{dt} = 0.50516\ \text{mH} \times 112{,}960\ \text{A/s} = 57.1\ \text{V}

3.5 Deterministic desynchronized ramping

ATESO enforces a facility-bus ramp cap of (dP/dt)bus ≤ 3.0 MW/ms. Socket release times are staggered deterministically across one AC cycle.

The 45 MW shed therefore arrives at 2.70 MW/ms, 10% inside the cap. A ramp spread over a full cycle limits high-frequency content in the step. Confirming that no network resonance is excited remains a site-specific frequency scan (P).


4. Frequency Regulation, Stability and Tariff Product Mapping

4.1 Dual-tier control architecture

4.2 Setpoints

Setpoint Value Basis
Tier 2 deadband 59.95–60.05 Hz, no modulation Design choice (P)
FFR trigger 59.85 Hz ERCOT FFR rule [4]
Full deployment 35–52 ms after trigger; ERCOT allows 15 cycles (250 ms) §4.1 (F), [4]
Margin to the first UFLS stage Trigger sits 0.55 Hz above 59.30 Hz [5]
For contrast: ERCOT under-frequency-relay Load Resources 59.70 Hz, 30 cycles [4]

4.3 Product mapping: the fifteen-minute compute-internal hold

ERCOT’s Fast Frequency Response requires full deployment within 15 cycles of a 59.85 Hz trigger. The resource must sustain the response for up to 15 minutes once deployed and restore within 15 minutes of recall [4]. ATESO meets the rule in three phases:

Phase Window Product Mechanism
1. Ingress Trip → one cycle (35–52 ms after 59.85 Hz, end to end) ERCOT FFR deployment Tier 1 trip; DVFS throttle of Class B cores; 45 MW at 2.70 MW/ms
2. Hold To 15 minutes ERCOT FFR sustainment Class B deferral inside the compute fabric; UPS on float
3. Restore After ERCOT recall Handoff to primary response and ECRS Class B resumes over minutes; ready to redeploy within 15 minutes
  1. Ingress. The shed lands within one cycle of the trip, before governors have delivered meaningful response.
  2. Hold. The 45 MW curtailment is sustained for the full fifteen minutes by deferring Class B work. No battery supplies it, and the UPS never leaves float, so the hold incurs zero cell cycling.
  3. Restore. Deferred work resumes at a grid-friendly pace agreed with the operator, for example 45 MW over five minutes. The 3.0 MW/ms cap governs electrical transients, not restoration. Re-adding 45 MW in a few milliseconds would itself be the shock load this paper sets out to remove. No work is dropped; deferred work completes later.

4.4 Modeled frequency arrest: the islanded system

We model Case A with the Anderson–Mirheydar system-frequency-response structure [20]: - H = 3.0 s, load damping D = 1, 5% droop; - a reheat turbine (FH = 0.3, TR = 8 s); - a governor lag and ERCOT’s ±36 mHz governor deadband.

A 100 MW step strikes at t = 0. CAVI responds per §4.1.

[Fig. 3 — 100 MW step on the 1 GVA island: modeled frequency (governor lag 0.3 s, ±36 mHz)]

  60.00 Hz ──┬───────────────────────────────────────────────────────────────
             │
  59.85 Hz ──┼── FFR trigger · crossed at 153 ms · 45 MW lands 35–52 ms later
             │
  59.54 Hz ──┼── Nadir with ATESO CAVI (t = 1.53 s) ····· 0.24 Hz above UFLS
             │
  59.30 Hz ──┼── First UFLS stage: 5% of load shed ──────────────────────────
  59.20 Hz ──┴── Nadir without CAVI (t = 1.69 s) ········ 0.10 Hz below UFLS
Governor model Nadir, unmanaged Nadir, with 45 MW CAVI
No lag, no deadband 59.32 Hz 59.62 Hz
0.2 s lag 59.27 Hz 59.59 Hz
0.2 s lag, ±36 mHz deadband 59.24 Hz 59.56 Hz
0.3 s lag, ±36 mHz deadband (Fig. 3) 59.20 Hz 59.54 Hz

Speed versus magnitude. The nadir arrives about 1.5 s after the step, so the 45 MW magnitude does most of the work. For the Fig. 3 case, the table shows the nadir against the delay before the shed begins, counted from the 59.85 Hz crossing:

Shed begins Nadir
0 cycles after crossing 59.541 Hz
3 cycles 59.539 Hz
15 cycles (ERCOT’s allowance) 59.513 Hz
30 cycles 59.436 Hz
60 cycles 59.252 Hz

Sub-cycle speed buys 28 mHz of margin over a response at ERCOT’s allowance. The one-cycle actuation is margin; the mechanism is magnitude delivered before the governors. Speed matters most where inertia is lowest and the nadir arrives soonest.

4.5 The bulk-system case: ERCOT

Take a low-inertia condition, Ek = 135 GW·s, and the loss of one South Texas Project unit (1,375 MW, half of ERCOT’s 2,750 MW design contingency [5]):

On the bulk system, one campus is a contributor, not an arrester. Its value is as a procured, fast, non-degrading reserve.

4.6 Arrest contribution and equivalent inertia

The arrest contribution. A shed ΔP sustained over a window Δt reduces the frequency decline accumulated over that window by:

Δfarrest=f0ΔPshedΔt2HsysSsys=60×45MW×0.1555s2×3.0s×1,000MVA=0.070Hz \Delta f_{\text{arrest}} \;=\; \frac{f_0\,\Delta P_{\text{shed}}\,\Delta t}{2\,H_{\text{sys}}\,S_{\text{sys}}} \;=\; \frac{60 \times 45\ \text{MW} \times 0.1555\ \text{s}}{2 \times 3.0\ \text{s}\times 1{,}000\ \text{MVA}} \;=\; 0.070\ \text{Hz}

This is the 1 GVA island case over a 155.5 ms window.

The struck metric. Earlier drafts reported a “local arrest” inertia of 30.0 s. That figure is withdrawn. Substituting Δfarrest back into the inertia formula returns Hsys·Ssys/Scampus = 3.0 × 1,000/100 = 30.0 s identically. It is the grid’s own stored energy restated on the campus base and says nothing about the campus.

The energy basis. Over the 155.5 ms window, the shed delivers 45 MW × 0.1555 s = 7.0 MW·s. A synchronous machine releases the same energy while frequency falls 0.5 Hz if it stores:

Eequiv=f0ΔPshedΔt2Δf=60×45×0.15552×0.5=420MW·s⇒HE=4.20s on a 100 MVA base E_{\text{equiv}} \;=\; \frac{f_0\,\Delta P_{\text{shed}}\,\Delta t}{2\,\Delta f} \;=\; \frac{60 \times 45 \times 0.1555}{2 \times 0.5} \;=\; 420\ \text{MW·s} \qquad\Rightarrow\qquad H_E = 4.20\ \text{s on a 100 MVA base}

That is the kinetic energy of a 105 MVA combustion-turbine generator with H = 4.0 s. It is 42% of a 250 MW unit with the same H.

The power basis. The shed’s 45 MW equals the full governor response of a 250 MW unit holding 18% headroom (250 × 0.18 = 45 MW). Under a 5% droop, that unit delivers 45 MW only after frequency has fallen 0.54 Hz, and over seconds. CAVI delivers it one cycle after the trip.

The caveat. Equivalent inertia depends on the window chosen. A synchronous machine releases energy only while frequency falls; a sustained shed keeps delivering. Measured over one second instead of 155.5 ms, the same shed corresponds to HE = 27.0 s on the same base. We therefore report CAVI as Fast Frequency Response, with inertia equivalents given only alongside their window.

4.7 Small-signal stability of the Tier 2 loop

The linearized Tier 2 controller, with gains on the campus base, is:

GCAVI(s)=ΔPCAVI(s)Δf(s)=Kdroop+sKinertial1+sτf,τf=20ms,Kdroop=25p.u.,Kinertial=2.0p.u. G_{\text{CAVI}}(s) \;=\; \frac{\Delta P_{\text{CAVI}}(s)}{\Delta f(s)} \;=\; \frac{K_{\text{droop}} + s\,K_{\text{inertial}}}{1 + s\,\tau_f}, \qquad \tau_f = 20\ \text{ms},\; K_{\text{droop}} = 25\ \text{p.u.},\; K_{\text{inertial}} = 2.0\ \text{p.u.}

Design specification (P). Where the loop gain crosses unity, as it can in a weak island, Tier 2 is tuned for: - a gain crossover near ωc = 18.2 rad/s (2.9 Hz); - a phase margin of 51.4°, against a requirement of more than 30°; - a damping ratio of ζ = 0.49 (0.495 to three places), against a requirement of more than 0.20.

For a second-order-equivalent loop, the damping ratio follows from the phase margin φm exactly:

ζ=12tan⁡ϕmcos⁡ϕm=sin⁡ϕm2cos⁡ϕm \zeta \;=\; \tfrac{1}{2}\tan\phi_m\sqrt{\cos\phi_m} \;=\; \frac{\sin\phi_m}{2\sqrt{\cos\phi_m}}

Verification on the reference island (R). We closed the loop around the §4.4 plant, converting the campus gains to the 1,000 MVA system base. - The loop gain never reaches unity (peak 0.34), so no crossover exists and the loop is stable with margin to spare. - Closing it moves the system’s frequency mode from a damping ratio of 0.96 to fully overdamped. All closed-loop poles are real: −51.3, −1.26 and −0.36 s−1.

Sub-synchronous interaction (P). The derivative path’s gain rises toward Kinertial/τf = 100 p.u. It is 57 p.u. at 5 Hz and 99 p.u. at 45 Hz, and the swing-equation plant is not valid in that band. - Excluding sub-synchronous resonance therefore requires an impedance-based scan against the actual network. - We recommend a second low-pass pole of about 2 Hz on the derivative path, so that the controller’s gain falls below the droop gain above a few hertz.

4.8 Products and standards


5. Scope and Limits


6. Conclusion: Turning the AI Grid Threat into a Grid Asset

The energy transition and the AI build-out cannot proceed on a collision course. If data centers remain volatile loads, utilities will keep slowing their interconnection.

The answer is not to buy $85 million of degradable chemistry for every campus. It is to recognize that most of a campus’s load is work that can wait a quarter of an hour, and to give the grid a runtime that knows which work that is.

ATESO’s resident binary structure and sub-millisecond admission loop let a campus act one cycle after the trip: - shed 45 MW of deferrable compute; - complete ERCOT’s Fast Frequency Response 5–7× inside the time allowed; - hold for fifteen minutes without touching a battery; - keep active users at full throughput.

On an island, that response keeps frequency above the first load-shedding stage. On the bulk system, it joins a fleet of fast reserves that never wear out.

The grid cannot sustain AI as a shock load. Computing must become the damper.


Appendix A: Claim Register

Claim Value Class Where
Island RoCoF, 100 MW step 1.00 Hz/s F §1.3
ERCOT critical / record-low inertia 100 / 130 GW·s V §1.3, [5]
ERCOT RoCoF, 100 MW step 0.023–0.030 Hz/s F §1.3
ERCOT RoCoF, 2,750 MW loss 0.64–0.83 Hz/s F §1.3
ERCOT first UFLS stage 59.3 Hz, 5% of load V [5]
ERCOT FFR rules 59.85 Hz, 15 cycles, 15-min sustain, 15-min restore V [4]
ERCOT NOG §2.3 as the governing section — U (author citation) [7]
Large-load queue ≈ 410 GW, ≈ 87% data centers (Mar 2026) V [6]
Generation/storage queues 2,061 GW US; 408 GW ERCOT; > 5 years median V [16]
Data-center load-loss event 1,500 MW (1,260 MW sustained), 10 Jul 2024 V [14]
AI training power swings Qualitative, production telemetry V [15]
BESS 100 MW / 200 MWh capital ≈ $85M V [18]
Class A / Class B shares 25–35% / 65–75% U §3.1
Campus load needed for 45 MW 60–69 MW F §3.1
Shed ramp 2.70 MW/ms (cap 3.0) F §3.5
Leakage inductance 0.505 mH F §3.4
Inductive transient 57.1 V; 0.72% of phase V; 0.060% of BIL F §3.4
Socket current 0.5625 A at 800 V; ≈ 562 A at 0.8 V; 0.034 A/µs F §3.3
Tier 1 end-to-end response 35–52 ms; 5–7× inside 250 ms F (estimator assumption); P until tested §4.1
Island nadirs 59.20–59.32 Hz unmanaged; 59.54–59.62 Hz with CAVI R §4.4
Speed vs magnitude 28 mHz from sub-cycle speed R §4.4
ERCOT bulk contribution 3.3% of a 1,375 MW loss; 0.306 → 0.296 Hz/s F §4.5
Arrest contribution 0.070 Hz over 155.5 ms (island) F §4.6
“30.0 s local arrest inertia” Withdrawn (identity) — §4.6
Energy-equivalent inertia 420 MW·s; HE = 4.20 s on 100 MVA (155.5 ms, 0.5 Hz basis) F §4.6
Power-basis equivalence 250 MW × 18% = 45 MW at a 0.54 Hz deviation (5% droop) F §4.6
Tier 2 specification ωc 18.2 rad/s, PM 51.4°, ζ = 0.49 P §4.7
Tier 2 on the reference island Loop gain ≤ 0.34; overdamped R §4.7
PJM regulation structure Single signal since 1 Oct 2025; Up/Down Oct 2026 V [12]
Texas SB 6 ≥ 75 MW: shutoff equipment, emergency disconnection V [13]
IEEE 2800 scope and clauses IBRs only; Clause 5 reactive/voltage; Clause 6 active power–frequency V [8]
Compute-internal 15-minute hold Class B deferral, UPS on float P §4.3

Appendix B: Frequency Model and Reproduction


References

Parent research

  1. B. DeCrow. ATESO & The Magma Runtime: The Thermodynamic Obsolescence of Document-Centric Execution for Continuous Spatial Compute. ManyMoats Research, 2026. USPTO Provisional App. 64/159,586 (Claims 5, 14, 15, 19).

Reliability standards and grid-operator sources

  1. NERC. BAL-003-2: Frequency Response and Frequency Bias Setting.
  2. NERC. PRC-006: Automatic Underfrequency Load Shedding.
  3. J. Matevosyan (ERCOT). Frequency Response and Ancillary Services in ERCOT. NERC workshop presentation. Covers FFR (59.85 Hz, 15 cycles, 15-minute sustain, 15-minute restore) and UFR Load Resources (59.70 Hz, 30 cycles). https://www.nerc.com/globalassets/our-work/workshops/5-3_matevosjana__pfr_ercot_frequency_response_and_ancillary_services.pdf
  4. ERCOT. Inertia: Basic Concepts and Impacts on the ERCOT Grid. April 2018. https://www.ercot.com/files/docs/2018/04/04/Inertia_Basic_Concepts_Impacts_On_ERCOT_v0.pdf
  5. ERCOT. Large Load update, Senate Committee on Business & Commerce. April 2026. https://www.ercot.com/files/docs/2026/04/01/ERCOT_LargeLoad_Update_April2026_B-C_-Hearing.pdf
  6. ERCOT. Nodal Protocols and Nodal Operating Guides: Fast Frequency Response provisions (NPRR 863; NOGRR 187).
  7. IEEE. Std 2800-2022: Interconnection and Interoperability of Inverter-Based Resources (IBRs) Interconnecting with Associated Transmission Electric Power Systems. https://standards.ieee.org/ieee/2800/10453/
  8. IEEE. Std 1547-2018: Interconnection and Interoperability of Distributed Energy Resources with Associated Electric Power Systems Interfaces.
  9. IEEE. Std C57.12.00: General Requirements for Liquid-Immersed Distribution, Power, and Regulating Transformers.
  10. NFPA. 855: Standard for the Installation of Stationary Energy Storage Systems.
  11. PJM. Regulation Redesign Phase 1 FAQ, with an independent summary by Modo Energy. https://www.pjm.com/-/media/DotCom/markets-ops/ancillary/regulation-redesign-phase-1-faq.ashx · https://modoenergy.com/research/en/pjm-regulation-market-redesign-2025-battery-impacts

Large loads, AI power and queues

  1. Utility Dive. Texas law gives grid operator power to disconnect data centers during crisis (SB 6, signed 20 June 2025). https://www.utilitydive.com/news/texas-law-gives-grid-operator-power-to-disconnect-data-centers-during-crisi/751587/
  2. NERC. Incident Review: Considering Simultaneous Voltage-Sensitive Load Reductions (event of 10 July 2024). https://www.nerc.com/pa/rrm/ea/Documents/Incident_Review_Large_Load_Loss.pdf
  3. E. Choukse et al. (Microsoft, a frontier lab, GPU vendor). Power Stabilization for AI Training Datacenters. arXiv:2508.14318, 2025. https://arxiv.org/abs/2508.14318
  4. Lawrence Berkeley National Laboratory. Queued Up: 2026 Edition (data through end of 2025; published 1 July 2026). https://emp.lbl.gov/news/backlog-power-plants-seeking-transmission-grid-connection-eased-somewhat-2025-amidst
  5. Lawrence Berkeley National Laboratory. Queued Up: 2024 Edition. https://emp.lbl.gov/sites/default/files/2024-04/Queued%20Up%202024%20Edition_1.pdf

Storage cost and power-system dynamics

  1. NREL. Cost Projections for Utility-Scale Battery Storage: 2025 Update. June 2025. https://docs.nrel.gov/docs/fy25osti/93281.pdf
  2. P. Kundur. Power System Stability and Control. McGraw-Hill, 1994.
  3. P. M. Anderson, M. Mirheydar. A low-order system frequency response model. IEEE Transactions on Power Systems 5(3), 1990.
← Return to Index Download Authoritative PDF ↓ View Independent Claim Card →